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We report the measured production rates of unstable isotopes $^9$Li and $^8$He produced by cosmic muon spallation on $^{12}$C using two identical detectors of the RENO experiment. Their beta-decays accompanied by a neutron make a…

Borexino, a liquid scintillator detector at LNGS, is designed for the detection of neutrinos and antineutrinos from the Sun, supernovae, nuclear reactors, and the Earth. The feeble nature of these signals requires a strong suppression of…

Xenon dual-phase time projections chambers (TPCs) have proven to be a successful technology in studying physical phenomena that require low-background conditions. With 40t of liquid xenon (LXe) in the TPC baseline design, DARWIN will have a…

Instrumentation and Detectors · Physics 2024-07-26 M. Adrover , L. Althueser , B. Andrieu , E. Angelino , J. R. Angevaare , B. Antunovic , E. Aprile , M. Babicz , D. Bajpai , E. Barberio , L. Baudis , M. Bazyk , N. Bell , L. Bellagamba , R. Biondi , Y. Biondi , A. Bismark , C. Boehm , A. Breskin , E. J. Brookes , A. Brown , G. Bruno , R. Budnik , C. Capelli , J. M. R. Cardoso , A. Chauvin , A. P. Cimental Chavez , A. P. Colijn , J. Conrad , J. J. Cuenca-García , V. D'Andrea , M. P. Decowski , A. Deisting , P. Di Gangi , S. Diglio , M. Doerenkamp , G. Drexlin , K. Eitel , A. Elykov , R. Engel , S. Farrell , A. D. Ferella , C. Ferrari , H. Fischer , M. Flierman , W. Fulgione , P. Gaemers , R. Gaior , M. Galloway , N. Garroum , S. Ghosh , F. Girard , R. Glade-Beucke , F. Glück , L. Grandi , J. Grigat , R. Größle , H. Guan , M. Guida , R. Hammann , V. Hannen , S. Hansmann-Menzemer , N. Hargittai , T. Hasegawa , C. Hils , A. Higuera , K. Hiraoka , L. Hoetzsch , M. Iacovacci , Y. Itow , J. Jakob , F. Jörg , M. Kara , P. Kavrigin , S. Kazama , M. Keller , B. Kilminster , M. Kleifges , M. Kobayashi , A. Kopec , B. von Krosigk , F. Kuger , H. Landsman , R. F. Lang , I. Li , S. Li , S. Liang , S. Lindemann , M. Lindner , F. Lombardi , J. Loizeau , T. Luce , Y. Ma , C. Macolino , J. Mahlstedt , A. Mancuso , T. Marrodán Undagoitia , J. A. M. Lopes , F. Marignetti , K. Martens , J. Masbou , S. Mastroianni , S. Milutinovic , K. Miuchi , R. Miyata , A. Molinario , C. M. B. Monteiro , K. Morå , E. Morteau , Y. Mosbacher , J. Müller , M. Murra , J. L. Newstead , K. Ni , U. G. Oberlack , I. Ostrovskiy , B. Paetsch , M. Pandurovic , Q. Pellegrini , R. Peres , J. Pienaar , M. Pierre , M. Piotter , G. Plante , T. R. Pollmann , L. Principe , J. Qi , J. Qin , M. Rajado Silva , D. Ramírez García , A. Razeto , S. Sakamoto , L. Sanchez , P. Sanchez-Lucas , J. M. F. dos Santos , G. Sartorelli , A. Scaffidi , P. Schulte , H. -C. Schultz-Coulon , H. Schulze Eißing , M. Schumann , L. Scotto Lavina , M. Selvi , F. Semeria , P. Shagin , S. Sharma , W. Shen , M. Silva , H. Simgen , R. Singh , M. Solmaz , O. Stanley , M. Steidl , P. L. Tan , A. Terliuk , D. Thers , T. Thümmler , F. Tönnies , F. Toschi , G. Trinchero , R. Trotta , C. Tunnell , P. Urquijo , K. Valerius , S. Vecchi , S. Vetter , G. Volta , D. Vorkapic , W. Wang , K. M. Weerman , C. Weinheimer , M. Weiss , D. Wenz , C. Wittweg , J. Wolf , T. Wolf , V. H. S. Wu , M. Wurm , Y. Xing , M. Yamashita , J. Ye , G. Zavattini , K. Zuber

While cosmic ray muons themselves are relatively easy to veto in underground detectors, their interactions with nuclei create more insidious backgrounds via: (i) the decays of long-lived isotopes produced by muon-induced spallation…

High Energy Physics - Phenomenology · Physics 2014-11-18 Cristiano Galbiati , John. F. Beacom

New generation dark matter experiments aim at exploring the 10e-9 - 10e-10 pb cross-section region for the WIMP-nucleon scalar interactions. Neutrons produced in the detector components are one of the main factors that can limit detector…

High Energy Physics - Phenomenology · Physics 2008-11-26 V. Tomasello , V. A. Kudryavtsev , M. Robinson

Neutrons produced in nuclear interactions initiated by cosmic-ray muons present an irreducible background to many rare-event searches, even in detectors located deep underground. Models for the production of these neutrons have been tested…

High Energy Physics - Experiment · Physics 2019-12-18 B. Aharmim , S. N. Ahmed , A. E. Anthony , N. Barros , E. W. Beier , A. Bellerive , B. Beltran , M. Bergevin , S. D. Biller , R. Bonventre , K. Boudjemline , M. G. Boulay , B. Cai , E. J. Callaghan , J. Caravaca , Y. D. Chan , D. Chauhan , M. Chen , B. T. Cleveland , G. A. Cox , R. Curley , X. Dai , H. Deng , F. B. Descamps , J. A. Detwiler , P. J. Doe , G. Doucas , P. -L. Drouin , M. Dunford , S. R. Elliott , H. C. Evans , G. T. Ewan , J. Farine , H. Fergani , F. Fleurot , R. J. Ford , J. A. Formaggio , N. Gagnon , K. Gilje , J. TM. Goon , K. Graham , E. Guillian , S. Habib , R. L. Hahn , A. L. Hallin , E. D. Hallman , P. J. Harvey , R. Hazama , W. J. Heintzelman , J. Heise , R. L. Helmer , A. Hime , C. Howard , M. Huang , P. Jagam , B. Jamieson , N. A. Jelley , M. Jerkins , C. Kéfélian , K. J. Keeter , J. R. Klein , L. L. Kormos , M. Kos , A. Kr\u , C. Kraus , C. B. Krauss , T. Kutter , C. C. M. Kyba , B. J. Land , R. Lange , J. Law , I. T. Lawson , K. T. Lesko , J. R. Leslie , I. Levine , J. C. Loach , R. MacLellan , S. Majerus , H. B. Mak , J. Maneira , R. D. Martin , A. Mastbaum , N. McCauley , A. B. McDonald , S. R. McGee , M. L. Miller , B. Monreal , J. Monroe , B. G. Nickel , A. J. Noble , H. M. O'Keeffe , N. S. Oblath , C. E. Okada , R. W. Ollerhead , G. D. Orebi Gann , S. M. Oser , R. A. Ott , S. J. M. Peeters , A. W. P. Poon , G. Prior , S. D. Reitzner , K. Rielage , B. C. Robertson , R. G. H. Robertson , M. H. Schwendener , J. A. Secrest , S. R. Seibert , O. Simard , D. Sinclair , P. Skensved , T. J. Sonley , L. C. Stonehill , G. Teš , N. Tolich , T. Tsui , R. Van Berg , B. A. VanDevender , C. J. Virtue , B. L. Wall , D. Waller , H. Wan Chan Tseung , D. L. Wark , J. Wendland , N. West , J. F. Wilkerson , J. R. Wilson , T. Winchester , A. Wright , M. Yeh , F. Zhang , K. Zuber

Ambient radiation background contributed by the penetrating cosmic ray particles and the radionuclides present in the rock materials have been measured at an underground laboratory located inside a mine at 555 m depth. The laboratory is…

Instrumentation and Methods for Astrophysics · Physics 2022-03-14 Sayan Ghosh , Shubham Dutta , Naba Kumar Mondal , Satyajit Saha

Cosmic-ray-muon spallation-induced radioactive isotopes with $\beta$ decays are one of the major backgrounds for solar, reactor, and supernova relic neutrino experiments. Unlike in scintillator, production yields for cosmogenic backgrounds…

High Energy Physics - Experiment · Physics 2016-01-20 Kamiokande Collaboration

In the published cosmogenic background study for a ton-sized DarkSide dark matter search, only prompt neutron backgrounds coincident with cosmogenic muons or muon induced showers were considered, although observation of the initiating…

Instrumentation and Methods for Astrophysics · Physics 2014-07-28 Anton Empl , Ed V. Hungerford

Experiments seeking to detect radio emission stemming from neutrino interactions will soon reach sensitivities that bring a detection within reach. Since experiments like RNO-G or the future IceCube-Gen2 target more than an order of…

High Energy Astrophysical Phenomena · Physics 2023-11-17 Lilly Pyras , Christian Glaser , Steffen Hallmann , Anna Nelles

The IceCube Neutrino Observatory is a cubic kilometer-sized detector designed to detect neutrinos of astrophysical origin. However, muons created by cosmic rays interacting in the atmosphere pose a significant background for these…

High Energy Astrophysical Phenomena · Physics 2021-07-22 Sarah Mancina , Manuel Silva

The IceCube neutrino detector is a cubic kilometer TeV to PeV neutrino detector under construction at the geographic South Pole. The dominant population of neutrinos detected in IceCube is due to meson decay in cosmic-ray air showers. These…

Astrophysics · Physics 2008-12-18 The IceCube Collaboration , A. Achterberg

Cosmic-rays with energies up to $3\times10^{20}$ eV have been observed. The nuclear composition of these cosmic rays is unknown but if the incident nuclei are protons then the corresponding center of mass energy is $\sqrt{s_{nn}} = 700$…

Nuclear Experiment · Physics 2009-11-18 Spencer R. Klein

In the case of underground experiments for neutrino physics or rare event searches, the background caused by cosmic muons contributes significantly and therefore must be identified and rejected. We proposed and optimized a new detector…

Instrumentation and Detectors · Physics 2017-04-05 Y. P. Zhang , J. L. Xu , H. Q. Lu , P. Zhang , C. C. Zhang , C. G. Yang

High-energy neutrinos, arising from decays of mesons that were produced through the cosmic rays collisions with air nuclei, form unavoidable background noise in the astrophysical neutrino detection problem. The atmospheric neutrino flux…

High Energy Astrophysical Phenomena · Physics 2010-10-13 S. I. Sinegovsky , A. A. Kochanov , T. S. Sinegovskaya

The solar neutrino experiment Borexino, which is located in the Gran Sasso underground laboratories, is in a unique position to study muon-induced backgrounds in an organic liquid scintillator. In this study, a large sample of cosmic muons…

The Jiangmen Underground Neutrino Observatory (JUNO) is a 20 kton liquid scintillator detector currently being built in a dedicated underground laboratory in China. It is a multi-purpose underground experiment with a physics program…

Instrumentation and Detectors · Physics 2022-03-02 Yongpeng Zhang

Cosmic muon interactions are important contributors to backgrounds in underground detectors when searching for rare events. Typically neutrons dominate this background as they are particularly difficult to shield and detect in a veto…

Instrumentation and Methods for Astrophysics · Physics 2012-10-10 A. Empl , R. Jasim , E. Hungerford , P. Mosteiro
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